Faraday's Electromagnetic Induction |
|||
Author(s): Aldo Cos & Tom Schuster | Demonstration Equipment
- Teacher's Guide SED 695B; Fall 2005 |
||
Principles illustrated: Electromagnetic Induction
|
|
||
Standards addressed: Physics 5f:
|
|||
Materials |
Explanation of principles involved
|
||
|
Students may wonder how transformers and generators work. Here is described a potential lab or demonstration of Faraday's principle of electromagnetic induction. Since the copper coils (refered to as a loop) contain a changing electric charge, an object placed within the electric field will become charged (magnetized). When the rod is pushed in and out of the coils, the magnetic field around the coils is changed. This in turn makes the electrons (current) in the coil move. This can be observed by the alternating (+) and (-) movements on the galvanometer. Alternatively, or additionally, the apparatus can be rearranged so that an electrical current generated from a battery is passed through the coil. The rod provides a direction for the current and stabilizes it. Furthermore, the rod becomes magnatized and can be used to pick up small metal objects, like paper clips. Background information: Faraday’s Law of Induction In words: The induced EMF (voltage or potential difference) around a closed loop is equal to the instantaneous rate of change (derivative) of the magnetic flux through the loop. In equation form: There are three ways to change the magnetic flux through a loop:
Therefore changing the angle either increases or decreases the flux because the dot product depends on the sine of the angle between the vectors B and dA. This is how a generator works. A generator rotates a loop (actually multiple loops) of wire through a fixed magnetic field and induces a voltage around the loop by rapidly changing the flux through the loop as it rotates. That induced voltage around the loops causes a current to flow through the wire and that is the output current of the generator. The negative sign indicates that the induced voltage is in a direction that creates a current that opposes the change in flux in the loop. This relationship is stated in Lenz’s Law. Lenz’s Law: The induced current in a loop of wire will be in a direction that opposes the change in flux through the loop. In other words, if the flux through the loop is being increased, then the induced current will create its own flux that will try to cancel out the increase in flux. If the flux through the loop is being decreased, then the induced current will be in a direction that tries to increase the flux through the loop. |
||
Procedure:
|
|||
References & Links:
|